Loading [MathJax]/jax/element/mml/optable/GeneralPunctuation.js
Research article

Rational solutions of an extended (2+1)-dimensional Camassa-Holm- Kadomtsev-Petviashvili equation in liquid drop

  • Received: 27 July 2022 Revised: 25 October 2022 Accepted: 30 October 2022 Published: 16 November 2022
  • MSC : 35A08, 35C05, 35C07, 35C08, 35C11

  • This paper investigates rational solutions of an extended Camassa-Holm-Kadomtsev-Petviashvili equation, which simulates dispersion's role in the development of patterns in a liquid drop, and describes left and right traveling waves like the Boussinesq equation. Through its bilinear form and symbolic computation, we derive some multiple order rational and generalized rational solutions and analyze their dynamic features, such as the connection between rational solution and bilinear equation, scatter behavior, moving path, and exact location of the soliton. The obtained solutions demonstrate two wave forms: multi-lump and multi-wave that consist of three, six and eight lump waves or two, three and four line waves. Moreover, different from the multi-wave solitons, stationary multiple dark waves are presented.

    Citation: Zhe Ji, Yifan Nie, Lingfei Li, Yingying Xie, Mancang Wang. Rational solutions of an extended (2+1)-dimensional Camassa-Holm- Kadomtsev-Petviashvili equation in liquid drop[J]. AIMS Mathematics, 2023, 8(2): 3163-3184. doi: 10.3934/math.2023162

    Related Papers:

    [1] Weaam Alhejaili, Mohammed. K. Elboree, Abdelraheem M. Aly . A symbolic computation approach and its application to the Kadomtsev-Petviashvili equation in two (3+1)-dimensional extensions. AIMS Mathematics, 2022, 7(11): 20085-20104. doi: 10.3934/math.20221099
    [2] Wafaa B. Rabie, Hamdy M. Ahmed, Taher A. Nofal, Soliman Alkhatib . Wave solutions for the (3+1)-dimensional fractional Boussinesq-KP-type equation using the modified extended direct algebraic method. AIMS Mathematics, 2024, 9(11): 31882-31897. doi: 10.3934/math.20241532
    [3] Junjie Li, Gurpreet Singh, Onur Alp İlhan, Jalil Manafian, Yusif S. Gasimov . Modulational instability, multiple Exp-function method, SIVP, solitary and cross-kink solutions for the generalized KP equation. AIMS Mathematics, 2021, 6(7): 7555-7584. doi: 10.3934/math.2021441
    [4] Abeer S. Khalifa, Hamdy M. Ahmed, Niveen M. Badra, Jalil Manafian, Khaled H. Mahmoud, Kottakkaran Sooppy Nisar, Wafaa B. Rabie . Derivation of some solitary wave solutions for the (3+1)- dimensional pKP-BKP equation via the IME tanh function method. AIMS Mathematics, 2024, 9(10): 27704-27720. doi: 10.3934/math.20241345
    [5] Boyu Wang . A splitting lattice Boltzmann scheme for (2+1)-dimensional soliton solutions of the Kadomtsev-Petviashvili equation. AIMS Mathematics, 2023, 8(11): 28071-28089. doi: 10.3934/math.20231436
    [6] Jamilu Sabi'u, Sekson Sirisubtawee, Surattana Sungnul, Mustafa Inc . Wave dynamics for the new generalized (3+1)-D Painlevé-type nonlinear evolution equation using efficient techniques. AIMS Mathematics, 2024, 9(11): 32366-32398. doi: 10.3934/math.20241552
    [7] Zheng Dou, Kexin Luo . Global weak solutions of nonlinear rotation-Camassa-Holm model. AIMS Mathematics, 2023, 8(7): 15285-15298. doi: 10.3934/math.2023781
    [8] Yaya Wang, Md Nurul Raihen, Esin Ilhan, Haci Mehmet Baskonus . On the new sine-Gordon solitons of the generalized Korteweg-de Vries and modified Korteweg-de Vries models via beta operator. AIMS Mathematics, 2025, 10(3): 5456-5479. doi: 10.3934/math.2025252
    [9] Ninghe Yang . Exact wave patterns and chaotic dynamical behaviors of the extended (3+1)-dimensional NLSE. AIMS Mathematics, 2024, 9(11): 31274-31294. doi: 10.3934/math.20241508
    [10] Yunxi Guo, Ying Wang . The Cauchy problem to a gkCH equation with peakon solutions. AIMS Mathematics, 2022, 7(7): 12781-12801. doi: 10.3934/math.2022707
  • This paper investigates rational solutions of an extended Camassa-Holm-Kadomtsev-Petviashvili equation, which simulates dispersion's role in the development of patterns in a liquid drop, and describes left and right traveling waves like the Boussinesq equation. Through its bilinear form and symbolic computation, we derive some multiple order rational and generalized rational solutions and analyze their dynamic features, such as the connection between rational solution and bilinear equation, scatter behavior, moving path, and exact location of the soliton. The obtained solutions demonstrate two wave forms: multi-lump and multi-wave that consist of three, six and eight lump waves or two, three and four line waves. Moreover, different from the multi-wave solitons, stationary multiple dark waves are presented.



    A classical dynamical system consists of a phase space M together with a unique function g, where, by iterating this function, we obtain the orbits of points. However, we can find many systems with some finite maps rather than a single map that acts on the phase space. Indeed, we can find many natural processes involved with two or more interactions whose evolutions evolve with discrete time [1,2]. Therefore, there is a need to extend the study of dynamical systems by considering more than one mapping. Mathematicians have studied such systems either as non-autonomous systems or as iterated function systems (IFS). Therefore, these systems originate from a common study, specifically, the study of classical dynamical systems. Hence, important concepts in dynamics, including transitivity and shadowing [3], could be extended to IFSs.

    In a dynamical system, generally, the future state follows from the initial state. Therefore, it is often deterministic. However, they often appear chaotic, i.e., minor changes in the initial state bring dramatically different long-term behavior. Both topological transitivity and shadowing are dynamical properties that are closely related to the chaoticity of dynamical systems. Usually, in chaos, topological transitivity is a part of its definition, or it is implied by it (at least in some spaces), or it implies chaos. Indeed, it is a part of the definition in Devaney's chaos [4], while in Li–Yorke chaos [5], if a function is topologically transitive (TT), then it is chaotic, but the converse is not valid. Moreover, a TT map g has points that eventually move under iteration from one arbitrary small neighborhood to any other. As a result, one cannot break the corresponding system into a pair of invariant subsystems under g. Recently, mathematicians have studied this property intensively since it is a global characteristic in the dynamical systems theory.

    Topological transitivity was introduced to dynamical systems by Birkhoff [6] in the 1920s. The term 'topologically transitive (TT)' is not a unified one. Instead, some authors use 'regionally transitive' [7,8], 'nomadic' [9], 'topologically ergodic' [10], cf. [8], and 'topologically indecomposable (or irreducible)' [11]. A mapping g of a dynamical system (M,g) is TT if, for any pair of non-empty open sets W1,W2M, there is some k>0 such that gk(W1)W2. The notion of topological transitivity was introduced to IFSs by Bahabadi in [3]. Devi and Mangang [12] have also discussed this notion in IFSs by giving several examples, and they also extend the notions of equicontinuity, sensitivity, and distality to IFSs. Moreover, Mangang [13] has studied the notions of mean equicontinuity, mean sensitivity, and mean distality of the product dynamical systems.

    A natural generalization of topological transitivity is chain transitivity. It connects any two points of the phase space by a chain with any desired error bound. It is an essential notion of a dynamical system. For example, if a dynamical system is chain transitive, then several shadowing properties, including thick shadowing and shadowing, are equivalent [14]. In a dynamical system, there might be a circumstance where for any error bound γ, we could not find a γ-chain but it may be simpler to obtain an η-average (or η-mean) chain with any average (or mean) error bound γ. It leads to the introduction of average (or mean) chain transitivity to dynamical systems.

    In dynamical systems theory, our main goal is to study the nature of all its orbits. Likewise, in IFSs, we study the orbit behaviors of the system. Yet, in particular cases, it is unlikely to compute the accurate initial value of a point, which gives rise to the approximate values of the orbits. Thus, we obtain pseudo-orbits of the system. The notion of shadowing puts these pseudo-orbits close to the actual orbits of the system. It was introduced independently by Anosov [15] and Bowen [16] in the 1970s. Shadowing plays an essential part in developing the qualitative theory of dynamical systems. In systems with shadowing property, any pseudo-orbit is followed uniformly by a true orbit over an arbitrarily long duration of time. Usually, it is crucial in systems with chaos, where even an arbitrarily small error in the initial position leads to a large divergence of orbits. Moreover, the shadowing lemma in [16] roughly states that shadowing is a common phenomenon in chaotic dynamical systems. In recent years, shadowing has developed intensively and has become a notion of great interest. Many researchers have introduced different aspects of shadowing in dynamical systems, including average shadowing [17], h-shadowing [18], ergodic shadowing [19], thick shadowing [20], and d-shadowing [20]. Consequently, these aspects of shadowing have also been extended to IFSs; for references, one can see, [3,21,22,23].

    Ruchi Das and Mukta Garg introduced the notions of average (or mean) chain properties and the almost average (or mean) shadowing property to dynamical systems in [24]. Unlike the classical shadowing property, the notion of the almost mean shadowing property deals with pseudo-orbits with very small mean errors. In [25], the authors have also investigated the chaotic behavior of maps with almost average (or mean) shadowing property.

    Motivated by this, in this work we wish to study the concepts of mean chain properties and the almost mean shadowing property in IFSs. In Section 2, we give some preliminary discussions on dynamical systems and IFSs. In Section 3, we introduce the notions of mean chain transitive (MCT), mean chain mixing (MCM), and totally mean chain transitive (TMCT) to IFSs and study the relations among them. We also give an example of an IFS that is not chain transitive (CT) but MCM (Example 3.5). In Section 4, we introduce the notion of almost mean shadowing property (AMSP) to IFSs and study some of its basic properties. We also study the relation between CT and AMSP in IFSs. In particular, in Theorem 4.7, we find that an IFS is CT if one of the constituent maps is surjective, and it has AMSP.

    We consider (M,g) to be a dynamical system where, (M,d) is a compact metric space and f is a self-continuous map on M. Put Z+={nZ:n0}}. Then the set O(s,g)={gn(s):nZ+} is said to be the orbit of sM under (M,g).

    Let (M,g) be a dynamical system. Let γ,η>0, then

    ⅰ) A finite sequence {s0,s1,,sn} in M is an η-chain if d(g(si),si+1)<η, 0in1. When i is not bounded above, it is called an η-pseudo-orbit.

    ⅱ) An η-pseudo-orbit {si}iZ+ is γ-shadowed by sM if d(gi(s),si)<γ, i0.

    A dynamical system (M,g) is said

    a) To have shadowing property (SP) if γ>0, η>0 such that every η-pseudo-orbit is γ-shadowed by some point in M.

    b) To be chain transitive (CT) if η>0, and for any pair of points s,tM, an η-chain joining s and t.

    c) To be chain mixing (CM) if η>0, and for any pair of points s,tM, N>0, such that nN, an η-chain joining s and t of length n.

    Hutchinson introduced IFSs in [26] and were popularized by Barnsley [27]. Moreover, Barnsley and Demko [28] first named the word IFS, and it has garnered much attention since then. Let Λ be a non-empty finite set; an IFS F={M;gα|αΛ} is a family of continuous mappings gα:MM, where αΛ, and (M,d) is a compact metric space. Put ΛZ+={αi:αiΛiZ+}. We use the short notation

    Fσi=gαi1gαi2gα1gα0.

    Let σ=αi be a typical member of ΛZ+. An infinite sequence {si}iZ+ in M is an orbit of F if σΛZ+, such that si=Fσi(s0), where Fσi(s0)=gαi1gαi2gα1gα0(s0) and Fσ0(s0)=s0. So, for any σΛZ+, we define Oσ(s)={Fσi(s):iZ+} as an orbit of sM related to σ. For an IFS F and for a fixed integer n>0, we define Λn={(α0,α1,,αn1):αiΛ,0in1}; fμ=gαn1gα1gα0; and Fn={fμ|μΛn}.

    Bahabadi [3] extended the notions of SP, average (or mean) SP (MSP), TT, CT and CM to IFSs. An IFS F is TT if for any pair of non-empty open sets W1,W2M, σΛZ+ such that Fσk(W1)W2 for some k0.

    Let F={M;gα|αΛ} be an IFS and let γ,η>0, then

    ⅰ) A finite sequence {s0,s1,,sn} in M is an η-chain if {α0,α1,,αn1} such that d(gαi(si),si+1)<η, 0in1. When i is not bounded above, it is called an η-pseudo-orbit.

    ⅱ) An η-pseudo-orbit {si}iZ+ is γ-shadowed by sM if σΛZ+ such that d(Fσi(s),si)<γ, i0.

    ⅲ) {si}iZ+ is an η-mean-pseudo-orbit if N>0, and σΛZ+ such that for any nN,

    1nn1i=0d(gαi(si),si+1)<η.

    ⅳ) An η-mean-pseudo-orbit {si}iZ+ is γ-mean shadowed by sM if

    lim supn1nn1i=0d(Fσi(s),si)<γ.

    An IFS F={M;gα|αΛ} is said

    a) To have SP if γ>0, η>0 such that every η-pseudo-orbit is γ-shadowed by a point in M.

    b) To be CT if η>0, and for any pair of points s,tM, an η-chain joining s and t.

    c) To be CM if η>0 and for any pair of points s,tM, N>0 such that nN, an η-chain joining s and t of length n.

    d) To have mean shadowing property (MSP) if γ>0, η>0 such that every η-mean-pseudo-orbit is γ-mean shadowed by a point in M.

    Mean chain properties and almost mean shadowing properties in dynamical systems have been introduced in [24]. The main aim of this paper is to extend these notions in IFSs. Therefore, we recall the following definitions in dynamical systems:

    Let η>0, a finite sequence {s0,s1,,sn} is an η-mean chain of length n if an integer 0<Pn such that Pmn,

    1mm1i=0d(g(si),si+1)<η.

    (M,g) is said to be mean chain transitive (MCT) if, for every η>0 and for any pair of points s,tM, an η-mean chain joining s and t. It is said to be totally mean chain transitive (TMCT) if gk is MCT for each k>0. And, it is said to be mean chain mixing (MCM) if for every η>0 and for any pair of points s,tM, an integer N>0 such that nN, an η-mean chain joining s and t of length n.

    Let η>0, a sequence {si}iZ+ is an almost η-mean pseudo-orbit of (M,g) if

    lim supn1nn1i=0d(g(si),si+1)<η.

    An almost η-mean pseudo-orbit {si}iZ+ is γ-mean shadowed by sM if

    lim supn1nn1i=0d(gi(s),si)<γ.

    (M,g) has almost mean shadowing property (AMSP) if for every γ>0, an η>0 such that every almost η-mean pseudo-orbit {si}iZ+ is γ-mean shadowed by a point in M. Throughout the paper, we consider (M,d) to be a compact metric space and gα:XX to be a continuous self-map in X for any αΛ.

    This section introduces the notions of mean chain transitivity (MCT), mean chain mixing (MCM), and totally mean chain transitivity (TMCT) to IFSs, and proves some preliminary results.

    Definition 3.1. Let η>0, a finite sequence {s0,s1,,sn} is an η-mean chain of length n if {α0,α1,,αn1} and an integer 0<Pn such that integer m with Pmn,

    1mm1i=0d(gαi(si),si+1)<η.

    Definition 3.2. An IFS F is considered to be MCT if for any η>0 and for any pair of points s,tM, an η-mean chain joining s and t.

    Definition 3.3. An IFS F is considered to be TMCT if Fk is MCT for each k>0.

    Definition 3.4. An IFS F is considered to be MCM if for any η>0 and for any pair of points s,tM, an integer N>0 such that nN, an η-mean joining s and t of length n.

    Following, we give an example of an IFS that is not CT but MCM.

    Example 3.5. Consider (M,d) to be a metric space with more than two elements, and let a,bM. Let g1,g2 be two self-maps in M defined by g1(s)=a and g2(s)=b for every sM. Then, the IFS, F={M;g1,g2} is not CT but MCM.

    Proof. Clearly, F is not CT, indeed for any pair s,tM with t{a,b}, there is no η-chain joining s and t with η<min{d(t,a),d(t,b)}. Now, we claim that F is MCM. Take η>0 and s,tM. For t{a,b}, it is obvious. Suppose t{a,b} and, let max{d(t,a),d(t,b)}=γ>0. Choose an integer N>0 for which N>γη. For every nN and a finite sequence {αi}n1i=0 where αi{1,2}, define si=Fσi(s) for 0in1 and sn=t. Then, for every integer m with Nmn, we have

    1mm1i=0d(gαi(si),si+1)<η.

    Thus, {si}ni=0 is an η-mean chain joining s and t of length n. Hence, F={M;g1,g2} is not CT but MCM.

    Theorem 3.6. Let F be an IFS. Then, F is MCT if Fk is MCT for some k>1.

    Proof. Let η>0 and let s,tM be two points. Let k>1 be fixed such that Fk is MCT. Then, there exists an η-mean chain {si}ni=0 of Fk joining s and t. Therefore, there exists a finite sequence {μ0,μ1,,μn1} and an integer 0<Pn such that integer m with Pmn,

    1mm1i=0d(fμi(si),si+1)<η (3.1)

    where fμi=gαik1gαik2gαi0 and μi={αi0,αi1,,αik1} for 0in1.

    For 0in, let

    tj={si,if j=ki,gαijki1gαijki2gαi0(si),if ki<j<(i+1)k,

    i.e.,

    {tj}nkj=0={t0=s,t1=gα00(s),t2=gα01gα00(s),,tk=s1,tk+1=gα10(s1),
    tk+2=gα11gα10(s1),,tnk1=gαn1k2gαn10(sn1),tnk=t}.

    Again, let

    {αj}nkj=0={α00,α01,,α10,α11,,α1k1,,αn1k2,αn1k1}.

    Then, integer l with nlnk, we have

    1ll1j=0d(gαj(tj),tj+1)1nnk1j=0d(gαj(tj),tj+1).

    For jik, the term vanishes, therefore

    1ll1j=0d(gαj(tj),tj+1)<1nn1i=0d(fμi(si),si+1).

    By using (3.1), we have

    1ll1j=0d(gαj(tj),tj+1)<η.

    Thus, {tj}nkj=0 is an η-mean chain joining s and t of length nk. Hence F is MCT.

    Theorem 3.7 shows that a TMCT IFS is MCM if the constituent maps are Lipschitz. A self-continuous function g on a metric space M is a Lipschitz function if L>0 such that d(g(s),g(t))Ld(s,t), s,tM.

    Theorem 3.7. Let F={M;gα|αΛ} be an IFS where each gα is a Lipschitz function. If F is MCM, then F is TMCT.

    Proof. Let k>1 be an integer, let η>0 and let s,tM be any pair of points. For each αΛ, as gα is Lipschitz, Lα>0 such that d(gα(u),gα(v))Lαd(u,v), u,vM. Let L=max{Lα:αΛ}. Then, d(gα(u),gα(v))Ld(u,v), αΛ and u,vM. Without loss of generality, let L1 and take γ=ηkLk1. Since F is MCM, N>0 such that nN, a γ-mean chain of F joining s and t of length n. Take an integer r>0 such that rkN. Then, we can get a γ-mean chain of F joining s and t of length rk, say {s0=s,s1,,srk=t}. Therefore, there exists an integer 0<Prk and a finite sequence, say {αi}rk1i=0={α00,α01,,α0k2,α0k1,α10,α11,,α1k2,α1k1,,αr1k2,αr1k1} such that integer m with Pmrk,

    1mm1i=0d(gαi(si),si+1)<γ. (3.2)

    Put γi=d(gαi(si),si+1) for 0irk1. Then, from Eq (3.2), we get

    1rkrk1i=0γi<γ. (3.3)

    Define ti=sik for 0ir. We claim that {t0,t1,,tr} is an η-mean chain of Fk joining s and t.

    Let fμi=gαik1gαik2gαi0 where μi={αi0,αi1,,αik1}, 0ir1. Then, 0ir1, we have

    d(fμi(ti),ti+1)=d(fμi(sik),s(i+1)k)=d(gαik1gαik2gαi0(sik),(s(i+1)k))d(gαik1gαik2gαi0(sik),gαik1gαik2gαi1(sik+1))++d(gαik1gαik2(s(i+1)k2),gαik1(s(i+1)k1))+d(gαik1(s(i+1)k1),s(i+1)k)Lk1γik++L2γ(i+1)k2+Lγ(i+1)k1<Lk1(γik++γ(i+1)k2+γ(i+1)k1).

    Therefore, using Eq (3.3), it is clear that

    1rr1i=0d(fμi(ti),ti+1)<1rLk1rk1i=0γi<Lk1kγ=η.

    Thus, {t0,t1,,tr} is an η-mean chain of Fk joining s and t. Hence, F is TMCT.

    Given two compact metric spaces (M,d) and (M,d), we take the metric space M×M with metric

    d

    and let \mathfrak{F} = \{M, g_\alpha|\alpha\in\Lambda\} and \mathfrak{G} = \{M'; g_\beta|\beta\in\Gamma\} be two IFSs.

    Then, we define the IFS, \mathfrak{F}\times\mathfrak{G} as

    \mathfrak{F}\times\mathfrak{G} = \{M\times M';h_{\alpha,\beta}|\alpha\in\Lambda,\beta\in\Gamma\},

    where h_{\alpha, \beta}(s, t) = (g_\alpha(s), g_\beta(t)) , \forall s\in M and t\in M' .

    Theorem 3.8. If \mathfrak{F} = \{M; g_\alpha|\alpha\in\Lambda\} is a MCM IFS, then \mathfrak{F}\times\mathfrak{F} is MCT.

    Proof. Let \eta > 0 and let (s, t), (u, v)\in M\times M be any two points.

    Since \mathfrak{F} is MCM and as \frac{\eta}{2} > 0 , there exist integers N_1, \; N_2 > 0 such that for any n_1\geq N_1 and n_2\geq N_2 , there are \frac{\eta}{2} -mean chains joining s and u , and joining t and v respectively.

    Put N = max \{N_1, N_2\} . Then, we can find two \frac{\eta}{2} -mean chains joining s and u , t and v respectively; say \{s_0 = s, s_1, \ldots, s_N = u\} and \{t_0 = t, t_1, \ldots, t_N = v\} . Therefore, there exist finite sequences \{\alpha_0, \alpha_1, \ldots, \alpha_{N-1}\} and \{\alpha_0^{'}, \alpha_1^{'}, \ldots, \alpha_{N-1}^{'}\} , and integers 0 < P_1, \; P_2\leq N such that \forall integers m', m'' with P_1\leq m'\leq N and P_2\leq m''\leq N , we have

    \frac{1}{m'}\sum\limits_{i = 0}^{m'-1}d(g_{\alpha_i}(s_i),s_{i+1}) < \frac{\eta}{2}

    and

    \frac{1}{m''}\sum\limits_{i = 0}^{m''-1}d(g_{\alpha_i^{'}}(t_i),t_{i+1}) < \frac{\eta}{2}.

    Take P = max \{P_1, \; P_2\} and consider \{(s_i, t_i)\}_{i = 0}^N . Then, \forall integer m with P\leq m\leq N , we have

    \begin{eqnarray*} \frac{1}{m}\sum\limits_{i = 0}^{m-1}d^{''}\left((g_{\alpha_i}(s_i),g_{\alpha_i^{'}}(t_i)),(s_{i+1},t_{i+1})\right) &\leq &\frac{1}{m}\sum\limits_{i = 0}^{m-1}d(g_{\alpha_i}(s_i),s_{i+1})+\frac{1}{m}\sum\limits_{i = 0}^{m-1} d(g_{\alpha_i^{'}}(t_i),t_{i+1})\cr & < &\frac{\eta}{2}+\frac{\eta}{2} = \eta. \end{eqnarray*}

    Thus, \{(s_i, t_i)\}_{i = 0}^N is an \eta -mean chain of \mathfrak{F}\times\mathfrak{F} joining (s, t) and (u, v) of length N . Hence, \mathfrak{F}\times\mathfrak{F} is MCT.

    Theorem 3.9. If \mathfrak{F} is a TMCT IFS, then \mathfrak{F}\times\mathfrak{F} is MCT.

    Proof. Let \eta > 0 and let (s, t), (u, v)\in M\times M be any two points. By definition of TMCT, we have \mathfrak{F} is MCT. Suppose, \{s_0 = s, s_1, \ldots, s_n = u\} and \{u_0 = u, u_1, \ldots, u_k = u\} are two \frac{\eta}{4} -mean chains respectively, joining s and u , and joining u to itself. Then, there exist finite sequences \{\alpha_0, \alpha_1, \ldots, \alpha_{n-1}\} and \{\alpha_0^{'}, \alpha_1^{'}, \ldots, \alpha_{k-1}^{'}\} and integers 0 < P_1\leq n and 0 < P_2\leq k such that

    \frac{1}{m}\sum\limits_{i = 0}^{m-1}d(g_{\alpha_i}(s_i),s_{i+1}) < \frac{\eta}{4}\forall \text { integer } m \text { with } P_1 \leq m \leq n \text {, }

    and

    \frac{1}{m'}\sum\limits_{i = 0}^{m'-1}d(g_{\alpha_i^{'}}(u_i),u_{i+1}) < \frac{\eta}{4}, \forall \text { integer } m^{\prime} \text { with } P_2 \leq m^{\prime} \leq k \text {. }

    In particular,

    \frac{1}{n}\sum\limits_{i = 0}^{n-1}d(g_{\alpha_i}(s_i),s_{i+1}) < \frac{\eta}{4},

    and

    \frac{1}{k}\sum\limits_{i = 0}^{k-1}d(g_{\alpha_i^{'}}(u_i),u_{i+1}) < \frac{\eta}{4}.

    From the definition of TMCT, \mathfrak{F}^k is MCT. Let \{t_0 = g_{\alpha_{n-1}}\circ\cdots\circ g_{\alpha_0}(t), t_1, \ldots, t_p = v\} be an \frac{\eta}{2} -mean chain of \mathfrak{F}^k joining g_{\alpha_{n-1}}\circ\cdots\circ g_{\alpha_0}(t) and v of length p . Therefore, we can find a finite sequence \{\mu_0, \mu_1, \ldots, \mu_{p-1}\} and an integer 0 < P\leq p such that

    \frac{1}{m''}\sum\limits_{i = 0}^{m''-1}d(f_{\mu_i}(t_i),t_{i+1}) < \frac{\eta}{2}, \forall \text { integer } m^{\prime \prime} \text { with } P \leq m^{\prime \prime} \leq p \text {, }

    where f_{\mu_i} = g_{\alpha_{k-1}^i}\circ g_{\alpha_{k-2}^i}\circ\cdots\circ g_{\alpha_{0}^i} and \mu_i = \{\alpha_{0}^i, \alpha_{1}^i, \ldots, \alpha_{k-1}^i\} for 0\leq i\leq p-1 .

    Consider

    \begin{align*} \{z_i\}_{i = 0}^{n+pk}& = \{t,g_{\alpha_0}(t),\ldots,g_{\alpha_{n-1}}\circ\cdots\circ g_{\alpha_0}(t)\\ & = t_0,g_{\alpha_{0}^0}(t_0),\ldots,g_{\alpha_{k-2}^0}\circ\cdots\circ g_{\alpha_{0}^0}(t_0),t_1,g_{\alpha_{0}^1}(t_1),\ldots,g_{\alpha_{k-2}^1}\circ\cdots\circ g_{\alpha_{0}^1}(t_1),t_2,g_{\alpha_{0}^2}(t_2),\\ &\ldots,t_{p-1},g_{\alpha_{0}^{p-1}}(t_{p-1}),\ldots,g_{\alpha_{k-2}^{p-1}}\circ\cdots\circ g_{\alpha_{0}^{p-1}}(t_{p-1}),t_p = v\} \end{align*}

    with respect to the finite sequence

    \begin{align*} \{\alpha_i^{''}\}_{i = 0}^{n+pk}& = \{\alpha_0,\alpha_1,\ldots,\alpha_{n-1},\alpha_{0}^0, \alpha_{1}^0,\ldots,\alpha_{k-1}^0,\alpha_{0}^1,\ldots, \alpha_{k-1}^1,\ldots,\alpha_{0}^{p-1},\ldots, \alpha_{k-1}^{p-1}\}. \end{align*}

    Then, it is clear that the term d(g_{\alpha_i^{''}}(z_i), z_{i+1}) vanishes whenever i\neq n+jk where 0 < j\leq p-1 . Therefore,

    \begin{eqnarray*} \frac{1}{n+pk}\sum\limits_{i = 0}^{n+pk-1}d(g_{\alpha_i^{''}}(z_i),z_{i+1})& = &\frac{1}{n+pk}\sum\limits_{i = 0}^{p-1}d(g_{\alpha_{k-1}^i}\circ g_{\alpha_{k-2}^i}\circ\cdots\circ g_{\alpha_{0}^i}(t_i),t_{i+1})\cr & = &\frac{1}{n+pk}\sum\limits_{i = 0}^{p-1}d(f_{\mu_i}(t_i),t_{i+1})\cr & < &\frac{1}{p}\sum\limits_{i = 0}^{p-1}d(f_{\mu_i}(t_i),t_{i+1})\cr & < &\frac{\eta}{2}. \end{eqnarray*}

    Thus, \{z_i\}_{i = 0}^{n+pk} is an \frac{\eta}{2} -mean chain of \mathfrak{F} joining t and v .

    Again, consider

    \{w_i\}_{i = 0}^{n+pk} = \{s_0 = s,s_1,\ldots,s_n = u = u_0,\underbrace{u_1,\ldots,u_k = u}_{p\; \text{times}},u_1,\ldots,u_k = u,\ldots,u_1,\ldots,u_k = u\}

    with respect to the finite sequence

    \{\alpha_i^{'''}\}_{i = 0}^{n+pk} = \{\alpha_0,\alpha_1,\ldots,\alpha_{n-1}, \underbrace{\alpha_0^{'},\alpha_1^{'},\ldots,\alpha_{k-1}^{'}}_{p\; \text{times}},\ldots,\alpha_0^{'},\alpha_1^{'},\ldots,\alpha_{k-1}^{'} \}.

    Now,

    \begin{eqnarray*} \frac{1}{n+pk}\sum\limits_{i = 0}^{n+pk-1}d(g_{\alpha_i^{'''}}(w_i),w_{i+1})& = &\frac{1}{n+pk}\left[\sum\limits_{i = 0}^{n-1}d(g_{\alpha_i}(s_i),s_{i+1})+p\sum\limits_{i = 0}^{k-1}d(g_{\alpha_i^{'}}(u_i),u_{i+1})\right]\cr & = &\frac{1}{n+pk}\sum\limits_{i = 0}^{n-1}d(g_{\alpha_i}(s_i),s_{i+1})+\frac{p}{n+pk}\sum\limits_{i = 0}^{k-1}d(g_{\alpha_i^{'}}(u_i),u_{i+1})\cr & < &\frac{1}{n}\sum\limits_{i = 0}^{n-1}d(g_{\alpha_i}(s_i),s_{i+1})+\frac{p}{pk}\sum\limits_{i = 0}^{k-1}d(g_{\alpha_i^{'}}(u_i),u_{i+1})\cr & < &\frac{\eta}{4}+\frac{\eta}{4}\cr & = &\frac{\eta}{2}. \end{eqnarray*}

    Thus, \{w_i\}_{i = 0}^{n+pk} is an \frac{\eta}{2} -mean chain of \mathfrak{F} joining s and u . This implies that \{(w_i, z_i)\}_{i = 0}^{n+pk} is an \frac{\eta}{2} -mean chain of \mathfrak{F}\times\mathfrak{F} joining (s, t) and (u, v) with respect to d^{''} . Hence, \mathfrak{F}\times\mathfrak{F} is MCT.

    This section introduces the notion of almost mean shadowing property (AMSP) to IFSs.

    Definition 4.1. Let \eta > 0 , a sequence \{s_i\}_{i\in\mathbb{Z}_+} is an almost \eta -mean pseudo-orbit of an IFS \mathfrak{F} if \exists \sigma\in\Lambda^{\mathbb{Z}_+} such that

    \limsup\limits_{n\rightarrow \infty}{\frac{1}{n}\sum\limits_{i = 0}^{n-1}d(g_{\alpha_i}(s_i),s_{i+1})} < \eta.

    An almost \eta -mean pseudo-orbit \{s_i\}_{i\in\mathbb{Z}_+} of an IFS \mathfrak{F} is \gamma -mean shadowed by s\in M if

    \limsup\limits_{n\rightarrow \infty}{\frac{1}{n}\sum\limits_{i = 0}^{n-1}d(\mathfrak{F}_{\sigma_i}(s),s_i)} < \gamma.

    Definition 4.2. An IFS \mathfrak{F} has AMSP if for any \gamma > 0 , \exists an \eta > 0 such that every almost \eta -mean pseudo-orbit \{s_i\}_{i\in\mathbb{Z}_+} is \gamma -mean shadowed by a point in M .

    Remark 4.3. From the definition, it is clear that AMSP implies MSP, but the converse may not be true.

    In the following, we give an example of an IFS that has MSP but does not have the AMSP.

    Example 4.4 Let (M, d) be the metric space as defined in [29, Example 9.1]. Let g_1, \; g_2 be self maps on M defined as

    \begin{gathered} g_1(p) = p,\; g_1(a_n) = a_{n+1},\; g_1(b_n) = b_{n+1},\\ g_2(p) = p,\; g_2(a_n) = a_n,\; g_2(b_n) = b_{n+1}. \end{gathered}

    Then, the IFS, \mathfrak{F} = \{M; g_1, g_2\} has MSP but does not have the AMSP.

    Proof. Proceeding similarly, as in the proof of [29, Theorem 9.2], it is clear that \mathfrak{F} has MSP.

    Also, in [24], it is given that (M, g_1) does not have the AMSP. So, for any \epsilon > 0 , we can find a \delta > 0 and an almost \delta -pseudo orbit with respect to \sigma = \{g_1, g_1, g_1, \cdots\} which is not \epsilon -shadowed in average by any point in M . Hence, the IFS \mathfrak{F} = \{M; g_1, g_2\} does not have the AMSP.

    Example 4.5. Let \mathfrak{F} be the IFS as defined in [30, Example 3.5]. Then, \mathfrak{F} , does not have MSP and AMSP.

    Proof. In [31, Remark 4.5], it has been given that \mathfrak{F} does not have MSP. Using, the above Remark 4.3, it is clear that \mathfrak{F} does not have the AMSP.

    Theorem 4.6. If \mathfrak{F} is an IFS with AMSP, then so does \mathfrak{F}^k for every k\geq2 .

    Proof. Let k\geq2 and \gamma > 0 . By hypothesis, \exists an \eta > 0 such that every almost \eta -mean pseudo-orbit is \frac{\gamma}{k} -mean shadowed by a point in M .

    Let \{t_i\}_{i\in\mathbb{Z}_+} be an almost \eta -mean pseudo-orbit of \mathfrak{F}^k . Then, \exists \sigma = \langle \mu_i\rangle such that \forall \mu_i\in\sigma

    \limsup\limits_{n\rightarrow \infty}{\frac{1}{n}\sum\limits_{i = 0}^{n-1}d(f_{\mu_i}(t_i),t_{i+1})} < \eta,

    where f_{\mu_i} = g_{\alpha_{k-1}^i}\circ g_{\alpha_{k-2}^i}\circ\cdots\circ g_{\alpha_{0}^i} and \mu_i = \{\alpha_0^i, \alpha_1^i, \ldots, \alpha_{k-1}^i\}\in\Lambda^k , \forall i\in\mathbb{Z}_+ .

    Now, for some \sigma^{'} = \langle\alpha_j^{'}\rangle = \{\alpha_0^0, \alpha_1^0, \ldots, \alpha_{k-1}^0, \alpha_0^1, \ldots\} , consider a sequence \{s_j\}_{j\in\mathbb{Z}_+} defined by

    s_j = \begin{cases} t_i, & \mbox{if } j = ki,\\ g_{\alpha_{j-ki-1}^i}\circ g_{\alpha_{j-ki-2}^i}\circ\cdots\circ g_{\alpha_0^i}(t_i), & \mbox{if } ki < j < (i+1)k. \end{cases}

    For ki < j < (i+1)k , we have 0 < l\leq k-1 such that s_j = s_{ik+l} = g_{\alpha_{l-1}^i}\circ g_{\alpha_{l-2}^i}\circ\cdots\circ g_{\alpha_0^i}(t_i) . Also, for any integer n > 0 , we can get some i\geq0 and 0 < l\leq k-1 for which n = ik+l . Thus,

    \begin{equation*} \limsup\limits_{n\rightarrow \infty}{\frac{1}{n}\sum\limits_{j = 0}^{n-1}d(g_{\alpha_j^{'}}(s_j),s_{j+1})} = \limsup\limits_{i\rightarrow \infty}{\frac{1}{ik+l}\sum\limits_{j = 0}^{ik+l-1}d(g_{\alpha_j^{'}}(s_j),s_{j+1})}. \end{equation*}

    For j\neq ki-1 , the term vanishes. Therefore,

    \begin{eqnarray*} \limsup\limits_{n\rightarrow \infty}{\frac{1}{n}\sum\limits_{j = 0}^{n-1}d(g_{\alpha_j^{'}}(s_j),s_{j+1})} & = &\limsup\limits_{i\rightarrow \infty}{\frac{1}{ik+l}\sum\limits_{j = 0}^{i-1}d(f_{\mu_j}(t_j),t_{j+1})}\cr &\leq&\limsup\limits_{i\rightarrow \infty}{\frac{1}{i}\sum\limits_{j = 0}^{i-1}d(f_{\mu_j}(t_j),t_{j+1})}\cr & < &\eta. \end{eqnarray*}

    This implies that \{s_j\}_{j\in\mathbb{Z}_+} is an almost \eta -mean pseudo-orbit of \mathfrak{F} with respect to \sigma^{'} . Therefore, \exists z\in M such that

    \limsup\limits_{n\rightarrow \infty}{\frac{1}{n}\sum\limits_{j = 0}^{n-1}d(\mathfrak{F}_{\sigma_j^{'}}(z),s_j)} < \frac{\gamma}{k}.

    Now,

    \begin{eqnarray*} \limsup\limits_{n\rightarrow \infty}{\frac{1}{n}\sum\limits_{i = 0}^{n-1}d(\mathfrak{F}_{\sigma_i}^k(z),t_i)} & = & \limsup\limits_{n\rightarrow \infty}{\frac{1}{n}\sum\limits_{i = 0}^{n-1}d(\mathfrak{F}_{\sigma_{ki}^{'}}(z),s_{ki})}\cr &\leq& \limsup\limits_{n\rightarrow \infty}{\frac{1}{n}\sum\limits_{i = 0}^{n-1}\sum\limits_{l = 0}^{k-1}d(\mathfrak{F}_{\sigma_{ki+l}^{'}}(z),s_{ki+l})}\cr & = &k\limsup\limits_{n\rightarrow \infty}{\frac{1}{nk}\sum\limits_{j = 0}^{nk-1}d(\mathfrak{F}_{\sigma_j^{'}}(z),s_j)}\cr & < &\gamma. \end{eqnarray*}

    Hence, \mathfrak{F}^k hasAMSP for every k\geq2 .

    Theorem 4.7. Let \mathfrak{F} = \{M; g_\alpha|\alpha\in\Lambda\} be an IFS, where one of the g_\alpha is surjective. If \mathfrak{F} has AMSP, then it is CT.

    Proof. Let \gamma > 0 and let s, t\in M be two points. Since \{g_\alpha:\alpha\in\Lambda\} is a family of uniformly continuous mappings, it is uniformly equicontinuous. Thus, \exists 0 < \eta < \gamma such that \forall u, v\in M and \forall \alpha\in\Lambda , d(g_\alpha(u), g_\alpha(v)) < \gamma whenever d(u, v) < \eta . By hypothesis, \mathfrak{F} has AMSP. Therefore, \exists \delta > 0 such that every almost \delta -mean pseudo-orbit of \mathfrak{F} is \frac{\eta}{2} -mean shadowed by a point in M .

    Let D = diam (M) and let K > 0 be an integer such that \frac{D}{K} < \delta . Suppose for a fixed \alpha^{*}\in\Lambda , g_{\alpha^{*}} is surjective. Then, we can easily see that g_{\alpha^{*}}^{-l}(t) exists \forall integer l with 0\leq l\leq K-1 .

    For i\in \mathbb{Z}_+ , fix an infinite sequence \sigma = \langle\alpha_i\rangle\in\Lambda^{\mathbb{Z}_+} . Again, for j\in\mathbb{Z}_+ , we consider an infinite sequence \{s_j\}_{j\in\mathbb{Z}_+} , where

    s_j = \begin{cases} \mathfrak{F}_{\sigma_{j-2iK}}, & \mbox{ } 2iK\leq j\leq (2i+1)K-1,\\ g_{\alpha^{*}}^{j-2(i+1)K+1}(t), & \mbox{ } (2i+1)K\leq j\leq2(i+1)K-1. \end{cases}

    For any \alpha'\in\Lambda , let us define \sigma^{'} = \langle\alpha_j^{'}\rangle\in\Lambda^{\mathbb{Z}_+} , where

    \alpha_j^{'} = \begin{cases} \alpha_{j-2iK}, & \mbox{ } 2iK\leq j\leq (2i+1)K-2,\\ \alpha', & \mbox{ } j = (2i+1)K-1,\\ \alpha^{*}, & \mbox{ } (2i+1)K\leq j \leq 2(i+1)K-2,\\ \alpha' & \mbox{ } j = 2(i+1)K-1. \end{cases}

    Now, for any n > 0 with iK\leq n\leq (i+1)K , we have

    \frac{1}{n}\sum\limits_{j = 0}^{n-1}d(g_{\alpha_j^{'}}(s_j),s_{j+1})\leq \frac{iD}{iK} = \frac{D}{K} < \eta.

    Therefore,

    \limsup\limits_{n\rightarrow \infty}{\frac{1}{n}\sum\limits_{j = 0}^{n-1}d(g_{\alpha_j^{'}}(s_j),s_{j+1})} < \eta.

    This implies that \{s_j\}_{j\in\mathbb{Z}_+} is an almost \delta -mean pseudo-orbit of \mathfrak{F} . By hypothesis, \exists z\in M such that

    \begin{equation} \limsup\limits_{n\rightarrow \infty}{\frac{1}{n}\sum\limits_{j = 0}^{n-1}d(\mathfrak{F}_{\sigma_j^{'}}(z),s_j)} < \frac{\eta}{2}. \end{equation} (4.1)

    Notice that, there exist infinitely many i\in\mathbb{Z}_+ for which there is some l with 2iK\leq l\leq (2i+1)K-1 , i.e., s_{l}\in\{s, \mathfrak{F}_{\sigma_1}(s), \mathfrak{F}_{\sigma_2}(s), \ldots, \mathfrak{F}_{\sigma_{K-1}}(s)\} such that d\left(\mathfrak{F}_{\sigma_{l}^{'}}(z), s_{l}\right) < \frac{\eta}{2} . Otherwise,

    \limsup\limits_{n\rightarrow \infty}{\frac{1}{n}\sum\limits_{j = 0}^{n-1}d(\mathfrak{F}_{\sigma_j^{'}}(z),s_j)}\geq\frac{\eta}{2}

    which contradicts (4.1).

    Similarly, the above statement holds when (2i+1)K\leq l\leq2(i+1)K-1 , i.e., s_{l}\in\{g_{\alpha^{*}}^{-(K-1)}(t), g_{\alpha^{*}}^{-(K-2)}(t), \ldots, g_{\alpha^{*}}^{-1}(t), t\} .

    Thus, we can find two integers l_1 and l_2 with 0 < l_1 < l_2 such that s_{l_1} = \mathfrak{F}_{\sigma_{p_1}}(s) for some 0\leq p_1\leq K-1 satisfying d\left(\mathfrak{F}_{\sigma_{l_1}^{'}}(z), s_{l_1}\right) < \frac{\eta}{2} and s_{l_2} = g_{\alpha^{*}}^{-p_2}(t) for some 0\leq p_2\leq K-1 satisfying d\left(\mathfrak{F}_{\sigma_{l_2}^{'}}(z), s_{l_2}\right) < \frac{\eta}{2} . Using the condition of equicontinuity, we have, d\left(g_{\alpha_{l_1}^{'}}(\mathfrak{F}_{\sigma_{l_1}^{'}}(z)), g_{\alpha_{l_1}^{'}}(s_{l_1})\right) < \gamma . This implies that d\left(\mathfrak{F}_{\sigma_{l_1+1}^{'}}(z), g_{\alpha_{l_1}^{'}}(s_{l_1})\right) < \gamma and d\left(\mathfrak{F}_{\sigma_{l_2}^{'}}(z), s_{l_2}\right) < \gamma . Therefore,

    \{s,\mathfrak{F}_{\sigma_1}(s), \mathfrak{F}_{\sigma_2}(s),\ldots, \mathfrak{F}_{\sigma_{p_1-1}}(s),\mathfrak{F}_{\sigma_{p_1}}(s) = s_{l_1},\mathfrak{F}_{\sigma_{l_1+1}^{'}}(z),

    \mathfrak{F}_{\sigma_{l_1+2}^{'}}(z), \ldots, \mathfrak{F}_{\sigma_{l_2-1}^{'}}(z), g_{\alpha^{*}}^{-p_2}(t) = s_{l_2}, g_{\alpha^{*}}^{-(p_2-1)}(t), \ldots, g_{\alpha^{*}}^{-1}(t), t\} is a \gamma -chain joining s and t with respect to the finite sequence \{\alpha_0, \alpha_1, \ldots, \alpha_{p_1-1}, \alpha_{l_1}^{'}, \alpha_{l_1+1}^{'}, \ldots, \alpha_{l_2-1}^{'}, \underbrace{\alpha^{*}, \alpha^{*}, \ldots\alpha^{*}}_{p_2\; \text{times}}\} . Hence, \mathfrak{F} is CT.

    In this work, we have introduced the notions of MCT, TMCT, MCM, and AMSP to IFSs and studied their interrelations. In Example 3.5, we have given an example of an IFS that is not CT but MCM. In Theorem 3.7, we proved that a TMCT IFS is MCM if the constituent maps are Lipschitz. For an iterated function system \mathfrak{F} , we show that \mathfrak{F}\times\mathfrak{F} is MCT if \mathfrak{F} is MCM. We also showed that \mathfrak{F}\times\mathfrak{F} is MCT if \mathfrak{F} is TMCT. Lastly, we prove that an IFS \mathfrak{F} , one of whose constituent maps g_\alpha is surjective and has AMSP, is CT.

    Thiyam Thadoi Devi: ideas, states, proof, and examples; Khundrakpam Binod Mangang: ideas, conceptualization, states, examples, and submission; Sonika Akoijam: states, proofs, and first draft; Lalhmangaihzuala: states, proofs, and edition; Phinao Ramwungzan: states, proofs, and examples; Jay Prakash Singh: revision and draft of the manuscript. All authors have read and approved the final version of the manuscript.

    The authors declare they have not used Artificial Intelligence (AI) tools in the creation of this article.

    We would like to thank the anonymous referees for their careful reading and valuable suggestions that have help us to improve the initial manuscript.

    The authors declare no conficts of interest.



    [1] L. Draper, 'Freak' ocean waves, Weather, 21 (1966), 2–4. https://doi.org/10.1002/j.1477-8696.1966.tb05176.x doi: 10.1002/j.1477-8696.1966.tb05176.x
    [2] P. Muller, C. Garrett, A. Osborne, Rogue waves, Oceanography, 18 (2005), 66–75. http://dx.doi.org/10.5670/oceanog.2005.30 doi: 10.5670/oceanog.2005.30
    [3] V. E. Zakharov, Stability of periodic waves of finite amplitude on the surface of a deep fluid, J. Appl. Mech. Tech. Phys., 9 (1968), 190–194. https://doi.org/10.1007/BF00913182 doi: 10.1007/BF00913182
    [4] A. Ankiewicz, N. Devine, N. Akhmediev, Are rogue waves robust against perturbations?, Phys. Lett. A, 373 (2009), 3997–4000. https://doi.org/10.1016/j.physleta.2009.08.053 doi: 10.1016/j.physleta.2009.08.053
    [5] N. Akhmediev, J. M. Soto-Crespo, A. Ankiewicz, Extreme waves that appear from nowhere: on the nature of rogue waves, Phys. Lett. A, 373 (2009), 2137–2145. https://doi.org/10.1016/j.physleta.2009.04.023 doi: 10.1016/j.physleta.2009.04.023
    [6] T. B. Benjamin, J. E. Feir, The disintegration of wave trains on deep water Part 1. Theory, J. Fluid. Mech., 27 (1967), 417–430. https://doi.org/10.1017/S002211206700045X doi: 10.1017/S002211206700045X
    [7] A. M. Turing, The chemical basis of morphogenesis, Bltn. Mathcal. Biology, 52 (1990), 153–197. https://doi.org/10.1007/BF02459572 doi: 10.1007/BF02459572
    [8] N. Akhmediev, A. Ankiewicz, J. M. Soto-Crespo, Rogue waves and rational solutions of the nonlinear Schrrödinger equation, Phys. Rev. E, 80 (2009), 026601. https://doi.org/10.1103/PhysRevE.80.026601 doi: 10.1103/PhysRevE.80.026601
    [9] W. X. Ma, Lump solutions to the Kadomtsev-Petviashvili equation, Phys. Lett. A, 379 (2015), 1975–1978. https://doi.org/10.1016/j.physleta.2015.06.061 doi: 10.1016/j.physleta.2015.06.061
    [10] S. F. Tian, D. Guo, X. B. Wang, T. T. Zhang, Traveling wave, lump wave, rogue wave, multi-kink solitary wave and interaction solutions in a (3+1)-dimensional Kadomtsev-Petviashvili equation with Bäcklund transformation, J. Appl. Anal. Comput., 11 (2021), 45–58. https://doi.org/10.11948/20190086 doi: 10.11948/20190086
    [11] Z. Y. Yin, S. F. Tian, Nonlinear wave transitions and their mechanisms of (2+1)-dimensional Sawada-Kotera equation, Physica D, 427 (2021), 133002. https://doi.org/10.1016/j.physd.2021.133002 doi: 10.1016/j.physd.2021.133002
    [12] Z. Y. Wang, S. F. Tian, J. Cheng, The \bar{\partial}-dressing method and soliton solutions for the three-component coupled Hirota equations, J. Math. Phys., 62 (2021), 093510. https://doi.org/10.1063/5.0046806 doi: 10.1063/5.0046806
    [13] X. Wang, L. Wang, C. Liu, B. W. Guo, J. Wei, Rogue waves, semirational rogue waves and W-shaped solitons in the three-level coupled Maxwell-Bloch equations, Commun. Nonlinear Sci., 107 (2022), 106172. https://doi.org/10.1016/j.cnsns.2021.106172 doi: 10.1016/j.cnsns.2021.106172
    [14] X. Wang, L. Wang, J. Wei, B. W. Guo, J. F. Kang, Rogue waves in the three-level defocusing coupled Maxwell-Bloch equations, Proc. R. Soc. A, 477 (2021), 20210585. https://doi.org/10.1098/rspa.2021.0585 doi: 10.1098/rspa.2021.0585
    [15] J. C. Chen, Z. Y. Ma, Y. H. Hu, Nonlocal symmetry, Darboux transformation and soliton-cnoidal wave interaction solution for the shallow water wave equation, J. Math. Anal. Appl., 460 (2018), 987–1003. https://doi.org/10.1016/j.jmaa.2017.12.028 doi: 10.1016/j.jmaa.2017.12.028
    [16] X. Wang, J. Wei, Three types of Darboux transformation and general soliton solutions for the space-shifted nonlocal PT symmetric nonlinear Schrödinger equation, Appl. Math. Lett., 130 (2022), 107998. https://doi.org/10.1016/j.aml.2022.107998 doi: 10.1016/j.aml.2022.107998
    [17] J. C. Chen, Z. Y. Ma, Consistent Riccati expansion solvability and soliton-cnoidal wave interaction solution of a (2+1)-dimensional Korteweg-de Vries equation, Appl. Math. Lett., 64 (2017), 87–93. https://doi.org/10.1016/j.aml.2016.08.016 doi: 10.1016/j.aml.2016.08.016
    [18] J. C. Chen, S. D. Zhu, Residual symmetries and soliton-cnoidal wave interaction solutions for the negative-order Korteweg-de Vries equation, Appl. Math. Lett., 73 (2017), 136–142. https://doi.org/10.1016/j.aml.2017.05.002 doi: 10.1016/j.aml.2017.05.002
    [19] X. Y. Gao, Y. J. Guo, W. R. Shan, Optical waves/modes in a multicomponent inhomogeneous optical fiber via a three-coupled variable-coefficient nonlinear Schrödinger system, Appl. Math. Lett., 120 (2021), 107161. https://doi.org/10.1016/j.aml.2021.107161 doi: 10.1016/j.aml.2021.107161
    [20] X. Y. Gao, Y. J. Guo, W. R. Shan, Taking into consideration an extended coupled (2+1)-dimensional Burgers system in oceanography, acoustics and hydrodynamics, Chaos Soliton. Fract., 161 (2022), 112293. https://doi.org/10.1016/j.chaos.2022.112293 doi: 10.1016/j.chaos.2022.112293
    [21] X. Y. Gao, Y. J. Guo, W. R. Shan, Similarity reductions for a generalized (3+1)-dimensional variable-coefficient B-type Kadomtsev-Petviashvili equation in fluid dynamics, Chinese J. Phys., 77 (2022), 2707–2712. https://doi.org/10.1016/j.cjph.2022.04.014 doi: 10.1016/j.cjph.2022.04.014
    [22] X. Y. Gao, Y. J. Guo, W. R. Shan, T. Y. Zhou, M. Wang, D. Y. Yang, In the atmosphere and oceanic fluids: scaling transformations, bilinear forms, Bäcklund transformations and solitons for a generalized variable-coefficient Korteweg-de Vries-modified Korteweg-de Vries equation, China Ocean Eng., 35 (2021), 518–530. https://doi.org/10.1007/s13344-021-0047-7 doi: 10.1007/s13344-021-0047-7
    [23] X. Y. Gao, Y. J. Guo, W. R. Shan, D. Y. Yang, Bilinear forms through the binary Bell polynomials, N solitons and Bäcklund transformations of the Boussinesq-Burgers system for the shallow water waves in a lake or near an ocean beach, Commun. Theor. Phys., 72 (2020), 095002. https://doi.org/10.1088/1572-9494/aba23d doi: 10.1088/1572-9494/aba23d
    [24] X. Y. Gao, Y. J. Guo, W. R. Shan, D. Y. Yang, Regarding the shallow water in an ocean via a Whitham-Broer-Kaup-like system: hetero-Bäcklund transformations, bilinear forms and M solitons, Chaos Soliton. Fract., 162 (2022), 112486. https://doi.org/10.1016/j.chaos.2022.112486 doi: 10.1016/j.chaos.2022.112486
    [25] R. Camassa, D. D. Holm, An integrable shallow water equation with peaked solitons, Phys. Rev. Lett., 71 (1993), 1661–1664. https://doi.org/10.1103/PhysRevLett.71.1661 doi: 10.1103/PhysRevLett.71.1661
    [26] Y. Zhang, H. Dong, X. Zhang, H. Yang, Rational solutions and lump solutions to the generalized (3+1)-dimensional shallow water-like equation, Comput. Math. Appl., 73 (2017), 246–252. https://doi.org/10.1016/j.camwa.2016.11.009 doi: 10.1016/j.camwa.2016.11.009
    [27] T. B. Benjamin, J. L. Bona, J. J. Mahony, Model equations for long waves in nonlinear dispersive systems, Phil. Trans. R. Soc. A, 272 (1972), 47–78. https://doi.org/10.1098/rsta.1972.0032 doi: 10.1098/rsta.1972.0032
    [28] A. Mekki, M. M. Ali, Numerical simulation of Kadomtsev-Petviashvili-Benjamin-Bona-Mahony equations using finite difference method, Appl. Math. Comput., 219 (2013), 11214–11222. https://doi.org/10.1016/j.amc.2013.04.039 doi: 10.1016/j.amc.2013.04.039
    [29] Y. Yin, B. Tian, X. Y. Wu, H. M. Yin, C. R. Zhang, Lump waves and breather waves for a (3+1)-dimensional generalized Kadomtsev-Petviashvili Benjamin-Bona-Mahony equation for an offshore structure, Mod. Phys. Lett. B, 32 (2018), 1850031. https://doi.org/10.1142/S0217984918500318 doi: 10.1142/S0217984918500318
    [30] D. J. Korteweg, G. de Vries, On the change of form of long waves advancing in a rectangular canal, and on a new type of long stationary waves, The London, Edinburgh, and Dublin Philosophical Magazine and Journal of Science, 39 (1895), 422–443. https://doi.org/10.1080/14786449508620739 doi: 10.1080/14786449508620739
    [31] Z. Liu, R. Wang, Z. Jing, Peaked wave solutions of Camassa-Holm equation, Chaos Soliton. Fract., 19 (2004), 77–92. https://doi.org/10.1016/S0960-0779(03)00082-1 doi: 10.1016/S0960-0779(03)00082-1
    [32] W. Liu, Y. Zhang, Families of exact solutions of the generalized (3+1)-dimensional nonlinear-wave equation, Mod. Phys. Lett. B, 32 (2018), 1850359. https://doi.org/10.1142/S0217984918503591 doi: 10.1142/S0217984918503591
    [33] J. P. Boyd, Peakons and cashoidal waves: travelling wave solutions of the Camassa-Holm equation, Appl. Math. Comput., 81 (1997), 173–187. https://doi.org/10.1016/0096-3003(95)00326-6 doi: 10.1016/0096-3003(95)00326-6
    [34] A. M. Wazwaz, A class of nonlinear fourth order variant of a generalized Camassa-Holm equation with compact and noncompact solutions, Appl. Math. Comput., 165 (2005), 485–501. https://doi.org/10.1016/j.amc.2004.04.029 doi: 10.1016/j.amc.2004.04.029
    [35] A. M. Wazwaz, The Camassa-Holm-KP equations with compact and noncompact travelling wave solutions, Appl. Math. Comput., 170 (2005), 347–360. https://doi.org/10.1016/j.amc.2004.12.002 doi: 10.1016/j.amc.2004.12.002
    [36] A. M. Wazwaz, Exact solutions of compact and noncompact structures for the KP-BBM equation, Appl. Math. Comput., 169 (2005), 700–712. https://doi.org/10.1016/j.amc.2004.09.061 doi: 10.1016/j.amc.2004.09.061
    [37] S. L. Xie, L. Wang, Y. Z. Zhang, Explicit and implicit solutions of a generalized Camassa-Holm Kadomtsev-Petviashvili equation, Commun. Nonlinear Sci., 17 (2012), 1130–1141. https://doi.org/10.1016/j.cnsns.2011.07.003 doi: 10.1016/j.cnsns.2011.07.003
    [38] A. Biswas, 1-Soliton solution of the generalized Camassa-Holm Kadomtsev-Petviashvili equation, Commun. Nonlinear. Sci., 14 (2009), 2524–2527. https://doi.org/10.1016/j.cnsns.2008.09.023 doi: 10.1016/j.cnsns.2008.09.023
    [39] C. Y. Qin, S. F. Tian, X. B. Wang, T. T. Zhang, On breather waves, rogue waves and solitary waves to a generalized (2+1)-dimensional Camassa-Holm-Kadomtsev-Petviashvili equation, Commun. Nonlinear Sci., 62 (2018), 378–385. https://doi.org/10.1016/j.cnsns.2018.02.040 doi: 10.1016/j.cnsns.2018.02.040
    [40] S. Y. Lai, Y. Xu, The compact and noncompact structures for two types of generalized Camassa-Holm-KP equations, Commun. Nonlinear Sci., 47 (2008), 1089–1098. https://doi.org/10.1016/j.mcm.2007.06.020 doi: 10.1016/j.mcm.2007.06.020
    [41] C. N. Lu, L. Y. Xie, H. W. Yang, Analysis of Lie symmetries with conservation laws and solutions for the generalized (3+1)-dimensional time fractional Camassa-Holm-Kadomtsev-Petviashvili equation, Comput. Math. Appl., 77 (2019), 3154–3171. https://doi.org/10.1016/j.camwa.2019.01.022 doi: 10.1016/j.camwa.2019.01.022
    [42] A. M. Wazwaz, Solving the (3+1)-dimensional KP-Boussinesq and BKP-Boussinesq equations by the simplified Hirota's method, Nonlinear Dyn., 88 (2017), 3017–3021. https://doi.org/10.1007/s11071-017-3429-x doi: 10.1007/s11071-017-3429-x
    [43] P. A. Clarkson, E. Dowie, Rational solutions of the Boussinesq equation and applications to rogue waves, Transactions of Mathematics and Its Applications, 1 (2017), tnx003. https://doi.org/10.1093/imatrm/tnx003 doi: 10.1093/imatrm/tnx003
    [44] D. E. Pelinovskii, Y. A. Stepanyants, New multisoliton solutions of the Kadomtsev–Petviashvili equation, JETP Lett., 57 (1993), 24–28.
    [45] Y. Y. Xie, L. F. Li, Multiple-order breathers for a generalized (3+1)-dimensional Kadomtsev-Petviashvili Benjamin-Bona-Mahony equation near the offshore structure, Math. Comput. Simulat., 193 (2021), 19–31. https://doi.org/10.1016/j.matcom.2021.08.021 doi: 10.1016/j.matcom.2021.08.021
  • This article has been cited by:

    1. Chander Bhan, Ravi Karwasra, Sandeep Malik, Sachin Kumar, Ahmed H. Arnous, Nehad Ali Shah, Jae Dong Chung, Bifurcation, chaotic behavior and soliton solutions to the KP-BBM equation through new Kudryashov and generalized Arnous methods, 2024, 9, 2473-6988, 8749, 10.3934/math.2024424
    2. Chong-Dong Cheng, Bo Tian, Tian-Yu Zhou, Yuan Shen, Nonlinear localized waves and their interactions for a (2+1)-dimensional extended Bogoyavlenskii-Kadomtsev-Petviashvili equation in a fluid, 2024, 125, 01652125, 103246, 10.1016/j.wavemoti.2023.103246
  • Reader Comments
  • © 2023 the Author(s), licensee AIMS Press. This is an open access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0)
通讯作者: 陈斌, bchen63@163.com
  • 1. 

    沈阳化工大学材料科学与工程学院 沈阳 110142

  1. 本站搜索
  2. 百度学术搜索
  3. 万方数据库搜索
  4. CNKI搜索

Metrics

Article views(1911) PDF downloads(141) Cited by(2)

Figures and Tables

Figures(21)

Other Articles By Authors

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return

Catalog